In La214, the electronic specific heat coefficient gamma (=C-el/T) is gradu
ally suppressed with lowering T below a certain temperature T* (> T-c), whe
re the in-plane resistivity rho and magnetic susceptibility chi also tend t
o be suppressed slightly. Temperature T*, increasing with lowering x, is in
qualitative agreement with the mean field T-c(T-co), estimated from the su
perconducting gap amplitude 2 Delta(0) at T much less than T-c, as the onse
t temperature T* of a pseudogap in Bi2212. The gradual suppression of gamma
below similar to T-co implies that a pseudogap will also open up below sim
ilar to T-co in La214 as in Bi2212. In underdoped samples, whose pseudogap-
like behaviors in C-el(T) become marked, the anomaly of C-el around T-c is
rather different from the BCS expectation.